Rongfeng Zhu

Mr. Rongfeng Zhu

Key Laboratory of Inorganic Functional Material and Device, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201800, China
+1
orcid

Research Focus & Metrics

Academic Career Length

8Years (2019-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 March 2020 in Journal of Alloys and Compounds
Verified
Journal Article
Closed access
JZJing Zhao
Jing Zhao
RZRongfeng Zhu
Rongfeng Zhu
QDQiuxiang Du
Qiuxiang Du
FLFei Liu
Fei Liu
YWYang Wu
Yang Wu
HLHaosu Luo
Haosu Luo

6 December 2019 in Journal of the American Ceramic Society
Verified
Journal Article
Closed access
PDF file
RZRongfeng Zhu
Rongfeng Zhu
JZJing Zhao
Jing Zhao
FLFei Liu
Fei Liu
ZZZhang Zhang
Zhang Zhang
Bijun FangBijun Fang
Bijun Fang
Haosu LuoHaosu Luo
Haosu Luo

4 June 2020 in Materials
Verified
Journal Article
Open access
PDF file
RZRongfeng Zhu
Rongfeng Zhu
JZJing Zhao
Jing Zhao
Jianwei ChenJianwei Chen
Jianwei Chen
Bijun FangBijun Fang
Bijun Fang
HXHaiqing Xu
Haiqing Xu
Haosu LuoHaosu Luo
Haosu Luo
Mn:0.15Pb(In1/2Nb1/2)O3-0.55Pb(Mg1/3Nb2/3)O3-0.30PbTiO3 (Mn:PIMNT) pyroelectric chips were prepared by a two-step annealing method. For the two steps, annealing temperatures dependence of microstructure, defects, surface stress, surface roughness, dielectric properties and pyroelectric properties were studied comprehensively. The controlling factors influencing the pyroelectric properties of the Mn:PIMNT crystals were analyzed and the optimum annealing temperature ranges for the two steps were determined: 600–700 °C for the first step and 500–600 °C for the second step. The pyroelectric properties of the thin Mn:PIMNT chips were significantly enhanced by the two-step annealing method via tuning oxygen vacancies and eliminating surface stress. Based on Mn:PIMNT pyroelectric chips annealed at the most favorable conditions (annealed at 600 °C for the first step and 500 °C for the second step), infrared detectors were prepared with specific detectivity D* = 1.63 × 109 cmHz1/2W−1, nearly three times higher than in commercial LiTaO3 detectors.